Electro-optical device and method of driving the same

ABSTRACT

The method of fine gradation display by an electro-optical device with little influence by difference in elemental devices, is disclosed, which is an object of the present invention. In case of an active matrix electro-optical device, a visual gradation display can be carried out by digitizing an analog image signal externally supplied by means of binary notation, by temporarily storing the digital signal thus obtained, by outputting the digital signal to a circuit of next step in a proper order, and by controlling the output timing of the signal so as to output the signal to the active matrix electro-optical device, and whereby digitally controlling the time for applying voltage to a picture element.

BACKGROUND OF THE INVENTION

1. Field of The Invention

The present invention relates to an electro-optical device and a methodof driving the same, and, in particular, to the method of gradationimage display for obtaining the expression having neutral color tone orintermediate brightness, by utilizing a thin film transistor(hereinafter referred to as TFT) as a switching device for driving. Thepresent invention relates, in particular, to the complete digitalgradation display for performing a gradation display without applyingany external analog signal to an active device.

2. Description of The Prior Art

A liquid crystal composition can easily be oriented in a paralleldirection or in a vertical direction to an external electric fieldexisting outside thereof, because the dielectric constant of the liquidcrystal composition in a direction parallel to the molecule axis thereofis different from that in a direction vertical to the molecule axis. TheON/OFF display, i.e. the display in a degree of brightness, is carriedout by taking advantage of the anisotropy in dielectric constant, andwhereby controlling the amount of transmitted light or the degree oflight dispersion. As a liquid crystal material, TN (twisted nematic)liquid crystal, STN (super-twisted nematic) liquid crystal,ferroelectric liquid crystal, antiferroelectric liquid crystal, polymerliquid crystal or dispersion liquid crystal are conventionally known. Itis known that it takes a certain period of time before a liquid crystalresponds to an external voltage, rather than an infinitely short periodof time. The value of the response time is proper to each liquid crystalmaterial: in case of TN liquid crystal, it is several 10 msec, while incase of STN liquid crystal, it is several 100 msec, and in case offerroelectric liquid crystal, it is several 10 microsec, while in caseof dispersion or polymer liquid crystal, it is several 10 msec.

Of the electro-optical device utilizing liquid crystal, a method ofobtaining the most excellent image quality is the one taking advantageof an active matrix method. In case of a conventional active matrix typeliquid crystal electro-optical device, a thin film transistor (TFT) wasused as an active device, while amorphous or polycrystallinesemiconductor was used for TFT, and either P-type or N-type TFT isutilized for one picture element. Namely, an N-channel TFT (alsoreferred to as NTFT) is generally connected to a picture element inseries. The NTFTs are provided at the intersections of the signal linesarranged in a matrix form. The ON/OFF of a liquid crystal pictureelement is controlled by taking advantage of the fact that a TFT isturned in an ON state when signals are applied to the TFT through thetwo signal lines connected thereto. By thus controlling the pictureelement, a liquid crystal electro-optical device of large contrast canbe achieved.

In case of the active matrix method as mentioned above, however,gradation display of brightness or color tone was very hard to carryout. Actually, a method utilizing the fact that the light transmissionof liquid crystal is varied dependent upon the level of voltage appliedthereto, was under examination. This meant, for example, that a properlevel of voltage was supplied between the source and the drain of theTFT in a matrix, from a peripheral circuit, and that the same level ofvoltage was applied to a liquid crystal picture element by applying asignal voltage to a gate electrode under the condition.

In case of the abovementioned method, however, the voltage actuallyapplied to the liquid crystal differed by at least several % inindividual picture elements, owing to inhomogeneity of the TFT or to theinhomogeneity of a matrix wiring. On the other hand, the voltagedependency of light transmission of a liquid crystal has an extremelystrong non-linear characteristic, and light transmission woulddrastically differs for the difference even by several % for the lighttransmission changes drastically at a certain voltage. For this reason,a 16 gradation was practically an upper limit.

For example, a voltage range of so-called transition region, that is avoltage range in which light transmission varies from ON state to OFFstate, is 1.2 V in case of TN liquid crystal material. Hence, in orderto achieve 16 gradations, a minute control of 75 mV voltages which arequotients of 1.2V divided by 16 is necessary and production yield hasbeen extremely low.

The difficulty in carrying out gradation display was an enormousdrawback of a liquid crystal display device in terms of competitivenesswith a CRT (cathode-ray tube) as a conventional and general displaydevice.

BRIEF SUMMARY OF THE INVENTION

An object of the present invention is to propose a completely novelmethod of gradation display which has been conventionally difficult.According to the present invention, an intermediate gradation display iscarried out not by applying an analog signal as has been in a prior art,but by applying a digital signal, and by means of the duration of theapplication. For this purpose, an analog image signal is digitizedthrough binary system calculation, and is stored in a memory device, andthe data is retrieved, calculated, and is outputted to a display device(an electro-optical device), as required. As a result of this, anadvanced gradation of no less than 16 gradations is achieved, which hasbeen extremely difficult by the prior art of analog gradation displaymethod.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows an example of a drive waveform in accordance with thepresent invention.

FIG. 2 shows an example of a drive waveform in accordance with thepresent invention.

FIG. 3 shows an example of a drive waveform in accordance with thepresent invention.

FIG. 4 shows an example of a drive waveform in accordance with thepresent invention.

FIG. 5 shows an example of a matrix form in accordance with the presentinvention.

FIG. 6 shows a schematic diagram of a device in accordance with thepreferred embodiment.

FIG. 7(A) to 7(F) show a process of TFT in accordance with the preferredembodiment.

FIG. 8(A) to 8(D) show a process of TFT in accordance with the preferredembodiment.

FIG. 9(A) to 9(F) show a process of TFT in accordance with the preferredembodiment.

FIG. 10(A) to 10(E) show a production process of a color filter inaccordance with the preferred embodiment.

FIG. 11 shows an example of the connection of a protection network.

FIG. 12(A) to 12(E) show examples of protection circuits.

FIG. 13(A) to 13(B) show examples of protection circuits.

FIG. 14 shows a block figure of an electro-optical device in accordancewith the present invention.

FIG. 15 shows a method of converting analog image data into digitalimage data in accordance with the present invention.

FIG. 16 shows an example of the order of data transfer in accordancewith the present invention.

FIG. 17 shows an example of the order of data transfer in accordancewith the present invention.

FIG. 18 shows an example of the order of data transfer in accordancewith the present invention.

FIG. 19 shows an example of a driving signal in accordance with thepresent invention.

FIG. 20 shows a block figure of a liquid crystal display device inaccordance with the preferred embodiment.

FIG. 21 shows a block figure of a liquid crystal display device inaccordance with the preferred embodiment.

FIG. 22 shows an example of a driving signal in accordance with thepreferred embodiment.

FIG. 23 shows an example of a matrix form in accordance with thepreferred embodiment.

FIG. 24 shows an example of a driving signal in accordance with thepreferred embodiment.

FIG. 25 is a copy of a photograph showing an electric circuit inaccordance with the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

As mentioned supra, the light transmission of a liquid crystal can becontrolled by controlling the voltage to be applied thereto, in ananalog mode, whereas the inventors have confirmed that a gradation canbe obtained visually by controlling the duration of voltage applied to aliquid crystal.

For example, in case of using a TN (twisted nematic) liquid crystalwhich is typically used as a liquid crystal material, it has beenconfirmed that the brightness can be varied by applying waveformvoltages as shown in FIG. 1 to a liquid crystal picture element designedto be in a normally black mode, i.e. non-light-transmittable state or ablack state, with no voltage applied to the picture element. Namely, itwill be gradually brighter in the order of numerals "1", "2", . . ."15", as shown in FIG. 1. In this way, a 16 gradation display ispossible according to the example shown in FIG. 1. In case of a normallywhite mode, which is a reverse mode of the normally black mode, andwhich is a light transmittable state with no voltage applied, thenumeral "1" should be the brightest while "15" the darkest.

At this time, a pulse of the length of one unit is applied at "1", whilea pulse of the length of two units is applied at "2" At "3", a one unitpulse and a two units pulse are applied, and thus a pulse of the lengthof three units is applied. At "4", a pulse of the length of four unitsis applied, while, at "5", a one unit pulse and a four-unit pulse areapplied. At "6", a two-unit pulse and a four-unit pulse are applied. Bypreparing a pulse of the length of eight units, a pulse of the length of15 units can consequently be obtained.

The display of 2⁴ =16 gradations will be achieved by properly couplingfour kinds of pulses of one unit, two-unit, four-unit, and eight-unit,with each other. Further, advanced gradation display of 32-gradation,64-gradation, 128-gradation, and 256-gradation will be achieved bypreparing pulses of 16-unit, 32-unit, 64-unit, and 128-unit,respectively. In order to obtain a 256 gradations display, for example,eight kinds of pulses are to be prepared.

As a suitable liquid crystal material in accordance with the presentinvention, TN (twisted nematic) liquid crystal, STN (super twistednematic) liquid crystal, ferroelectric liquid crystal, antiferroelectricliquid crystal, and dispersion or polymer liquid crystal, and so on, areto be used. The pulse width of one unit will be somewhat different fordifferent liquid crystal materials as mentioned supra: it has beenconfirmed that the suitable pulse width for TN liquid crystal is no lessthan 10 nsec-and no more than 100 msec.

In order to implement the present invention, for example, a matrixcircuit (an active matrix device) utilizing a thin film transistor asshown in FIG. 5 is to be formed. The circuit shown in FIG. 5 is the sameas the one used for an active matrix display device utilizing aconventional TFT. An example of one picture element of such an activematrix display device is shown in FIG. 6. Referring to this figure, aregion 63 designates, for example, a NTFT or PTFT comprisingpolysilicon, while an electrode 66 is a corresponding gate electrode. Awiring 65 is a gate wiring, which serves as X-line, while a wiring 74 isconnected with the source of TFT, and serves as Y-line. A wiring 68 isfor forming a capacitor shown in FIG. 5, which is provided under apicture element electrode 71 through an insulator.

Referring to FIG. 5, a capacitor is intentionally inserted in parallelwith the capacitor of a picture element. The capacitor thus inserted hasthe effect of suppressing the reduction in the voltage of the pictureelement due to natural discharge of the picture element, while it hasalso the effect of suppressing the fluctuation of the electric potentialof a picture element electrode due to the fluctuation of the electricpotential of X-line, caused by the capacitive coupling of the pictureelement electrode and the X-line through the parasitic capacitygenerated between a gate electrode and a drain region.

With regard to the latter effect, in particular, the degree of electricpotential fluctuation is approximately proportional to the parasiticcapacity between a gate and source or drain in an approximation, andinverse-proportional to the capacity of a liquid crystal pictureelement. The capacity of a picture element can be controlled relativelyeasily with a liquid crystal display device, whereas the difference inparasitic capacity tends to be widened, and, when the capacity of aliquid crystal picture element is small, as in the case when the area ofa liquid crystal unit picture element is small, the influence of thedifference in the parasitic capacity of a gate would be so large thatthe brightness would be completely at random for each picture element.This problem is critical when a gradation display is to be performed onthe presumption that the voltage applied to a picture element and theduration thereof are stable, particularly, for the implementation of thepresent invention. It is thus important, to increase the apparentcapacity of a liquid crystal picture element by inserting capacity inthis manner, and to reduce the fluctuation of the electric potential ofthe liquid crystal by suppressing the effect of the parasitic capacityof a gate.

A stable actuation of good reproducibility can be achieved withoutinserting this kind of intentional capacitor, by including an organicferroelectric material such as tetrafluoroethylene, polyvinylidenefluoride in a picture element of such as a liquid crystal cell so as toincrease the electrostatic capacity of the picture element, and wherebyincreasing the time constant of the discharging of the picture element.

It is not preferred, however, to add excessive capacity, since theadding of the capacitor in this way can lead to a reduction inoperational velocity. The level of the capacity to be added should bearound 10-100 times as large as the parasitic capacity of a gate, orseveral to 100 times as large as, or preferably no more than 10 times ofthe capacity proper to a liquid crystal picture element.

In the circuit as described above, the ON/OFF control of the voltageapplied to a picture element can be achieved by controlling the gatevoltage of each thin film transistor, and the voltage between the sourceand drain. In this example, a matrix is640×480 dots, however, only thevicinity of a n-th row and a m-th column is shown, to avoid complexity.A complete matrix can be obtained by developing the same patternvertically and horizontally. An example of operation using this circuit,is shown in FIG. 2.

Signal lines X₁, X₂ . . . X_(n), X_(n+1) . . . X₄₈₀ (hereinaftercollectively referred to as X-line) are connected with gate electrodesof TFTs. Rectangular pulse signals are applied thereto in turn, as shownin FIG. 2. On the other hand, signal lines Y₁, Y₂ . . . Y_(m), Y_(m+1) .. . Y₆₄₀ (hereinafter collectively referred to as Y-line) are connectedwith the source or drain electrodes of TFTs, to which a signalcomprising a plurality of pulses is applied. In this pulse train, 480pieces of information are included in one unit of time T₁.

In the following example, four picture elements Z_(n),m, Z_(n+1),m,Z_(n),m+1, Z_(n+1),m+1 are paid attention to, and, since the voltage ofthe picture element will not be changed unless signals are applied bothto a gate electrode and to a source electrode, signal lines X_(n),X_(n+1), Y_(m), and Y_(m+1) are to be paid attention to, in relation tothese four picture elements.

It is presumed that a rectangular pulse is applied to X_(n), as shown inthe figure. While the four picture elements Z_(n),m , Z_(n+1),m,Z_(n),m+1, and Z_(n+1),m+ are now paid attention to, correspondingstates of Y_(m) as well as of Y_(m+1) are to be paid attention to. Sincethere is a signal at Y_(m) and there is no signal at Y_(m+1), a pictureelement Z_(n),m+1 will be in voltage state (high voltage level), andZ_(n),m+1 will be in non-voltage state (low voltage level, e.g. zerolevel). By cutting the pulse of X-line, earlier than a voltage appliedto Y-line, the voltage state of the picture element is maintained by thecapacitor thereof, and thus the voltage state of the picture elementZ_(n),m will be maintained. In principle, the state of each pictureelement will be maintained until a next signal is applied to X_(n).

An additional pulse is applied to X_(n+1). Since Y_(m) is in non-voltagestate and Y_(m+1) in voltage state at the time, as shown in the figure,the picture element Z_(n+1),m will be in non-voltage state, whileanother picture element Z_(n+1),m+1 will be in voltage state, and thestate of each picture element is maintained as mentioned above.

When a second pulse is applied to a signal line X_(n) after a time T₁has passed since a preceding pulse was applied thereto, the state of thepicture element Z_(n),m+1 is changed into non-voltage state, and that ofthe picture element Z_(n),m+1 is changed into voltage state, for Y_(m)is in non-voltage state and Y_(m+1) in voltage state. An additionalpulse is applied to X_(n+1). Since both Y_(m) and Y_(m+1) are in voltagestate at the time, as shown in the figure, both of the picture elementsZ_(n+1),m and Z_(n+1),m+1 will be in voltage state. The voltage state ofthe picture element Z_(n+1),m+1 will be continued thereby.

A third signal is applied to X_(n) after a time 2T₁ has passed. Thistime, since both Y_(m) and Y_(m+1) are in voltage state, the pictureelement Z_(n),m+1 will be changed from non-voltage state into voltagestate, and the voltage state of the picture element Z_(n),m+1 will becontinued. An additional pulse is applied to X_(n+1). Since both Y_(m)and Y_(m+1) are in non-voltage state at the time, both of the pictureelements Z_(n+1),m and Z_(n+1),m+1 will be in non-voltage state, and thevoltage state for each is thus completed.

A fourth signal is then applied to X_(n) after a time 4T₁ has passed.Since both Y_(m) and Y_(m+1) are in non-voltage state at the time, bothof the picture elements Z_(n),m+1 and Z_(n),m+1 will be changed fromvoltage state into non-voltage state. An additional pulse is applied toX_(n+1), and, since both Y_(m) and Y_(m+1) are in non-volt age state,both of the picture elements Z_(n+1),m, and Z_(n+1),m+1 continue to bein non-voltage state.

In this manner, one cycle is completed. In this period of time, threepulses are applied to each X-line, while 3×480=1440 information signalsare applied to each Y-line. The period of time of the one cycle is 7T₁,and as a T₁, for example, 10 nsec-10 msec is appropriate. When eachpicture element is paid attention to, a pulse of the time T₁ as well asa pulse of the time 4T₁ are applied to the picture element Z_(n),m, andconsequently, the same effect as when a pulse of 5T₁ is applied, isobtained visually. Namely, a brightness of the grade "5" is obtained. Inthe same manner, the brightnesses of "2", "8" and , "3" are obtained forthe picture elements Z_(n),m+1, Z_(n+1),m, and Z_(n+1),m+1,respectively.

While an 8 gradations display is achieved in the above example, advancedgradation can be achieved by adding more pulse signals. Advancedgradation display of as many as 256 gradations will be achieved byapplying additional five pulses, for example, to each X-line andapplying 8×480=3840 information signals to each Y-line during one cycle.

An example of the arrangement is shown in FIGS. 1 and 2, where theduration of the voltage applied to a picture element is increased in ageometrical progression in such a way that it is first T₁, then 2 T₁,and then 4T₁, whereas this arrangement may be altered in such a way thatit is first T₁, then 8T₁, and then 2 T₁, and finally 4T₁, as shown inFIG. 3. The arrangement of the duration of the voltage shown in FIG. 3can be obtained by applying pulses (rectangular pulses to a signal line(X-line) at intervals, wherein said intervals are T₁ between the i-thpulse and the (i+1)-th pulse 2^(N) T₁ between the (i+1)-th pulse and the(i+2)-th pulse, 2^(N) T₁ between the (i+2)-th pulse and the (i+3)-thpulse and 2^(N-1) T₁ between the (i+3)-th pulse and the (i+4)-th pulsewhere i is a natural number and T₁ is a constant period and n is 3 inthis case. An example of a signal for driving in a way as illustrated inFIG. 3, is shown in FIG. 4. The number of pulses to be applied to X-lineper one screen is three, which is the same as for the case shown in FIG.2, while the time between pulses is first T₁, then 4T₁, and finally 2T₁.In this manner, the brightnesses of "3", "4", "6", and "5", areobtained, for example, for the picture elements Z_(n),m, Z_(n),m+1,Z_(n+1),m, and for Z_(n+1),m+1, respectively. By adopting a displaymethod of coupling long and short pulses with each other as shown inFIG. 3 or in FIG. 4, the operation of data transmission is facilitated.The structure of a peripheral circuit including the data transmissionwill be set forth in the following description.

A display device main body for implementing the present invention, andthe condition of a peripheral circuit thereof, are illustrated in FIG.14. A matrix size of a screen is as small as 8×8, for the purpose ofsimplification. The present invention is characterized by adding a FirstIn First Out memory device (hereinafter referred to as FIFO) on theexternal part of the driver of Y-line. Namely, the data to be suppliedto Y-line is temporarily stored by FIFO, and is then outputted toY-line, i.e. a display device. The data to be applied to Y-line has beenan analog signal according to a prior art, whereas a digital signal isused in accordance with the present invention. In a sense, it can besaid that FIFO can be added because the signal can be digitized. Byadding FIFO, the flowing of the signals can be averaged, and thus theburden on a driving circuit before a shift register as shown in FIG. 14,can be alleviated.

The terminology the burden on the driving circuit can be explained inthe following manner. When a signal of Y-line shown in FIG. 4 is paidattention to, as many as 480 information signals are applied to Y-lineduring first T₁. Although other 480 signals are applied during thefollowing 4T₁, the density of the signal is one-fourth of the firstbecause the duration is four times as long as that of the first. Thedensity of a signal during the following 2T₁ is a half of the first.When there is unevenness in the density of the signals, a circuit shouldbe designed based on the case of highest density. It is thus requiredthat 480 signals are processed by a shift register during T₁.

When the data during T₁ as well as the data during the next 4T₁ aretransmitted at the same time, since there are 980 signals in the timeperiod of 5T₁, 192 data are to be transmitted during one T₁. Byproviding FIFO, and whereby temporarily storing the data, the burden onthe shift register can be alleviated. This can be compared to a dam,into which a constant flow rate of water is flowed, and in which aconstant amount of water is accumulated therein, and thus the dam canflexibly discharge a large amount of water at a time or graduallydischarge a small amount. N-th image signal is outputted on an activematrix electro-optical device with (N+1)-th and (N+2)-th image signalsstored in a first in first out memory device connected to said activematrix electro-optical device during duration of said N-th image signalon said active matrix electro-optical device.

Referring to FIG. 14, fine timings of the FIFO and the shift registersfor X-lines and Y-lines are controlled by a logic sequencer.

An example of how a projected signal is processed is described infra. Asignal input as a normal analog image signal is immediately digitized bybinary notation calculation process, as shown in FIG. 15. The signal isconverted into, for example, a digital signal of 8-bit, or aneight-digit number. In this example, numeral 10 of analog signal, forexample, is converted into 00011001, and numeral 20 into 00110011, ornumeral 100 into 11111111. By converting into an 8-bit signal, thedisplay of 2⁸ =258 gradations is achieved. In the same manner, when 64gradations or 16 gradations are required, the analog signal is convertedinto 8-bit, or 4-bit signals, respectively. When a 128-gradation isrequired, it is converted into a 7-bit signal, or a seven-digit number.

The signal thus converted is temporarily stored in a memory. Each datais not stored as a group of data of 8-bit, but is distributed to and isstored in a memory of digital data for gradation display, as a datadistributed to total eight places of each digit of 8-bit, i e 2⁰, 2¹,2², 2³, 2⁴, 2⁵, 2⁶, and 2⁷, namely as a two-dimensional data of #0, #1,#2, #3, #4, #5, #6, and #7. The digital binary signal of each of the 8digits is stored into corresponding one of memory areas. When the dataof a first line and a second column of a matrix is required, a first row(line) and a second column of each data of #0-#7 bits is to be read. Inthis case, the data of 0, 0, 0, 1, 1, 0, 0, 1, is stored in this orderfrom #7. A gradation data is thus 00011001, and when this is convertedinto analog mode in decimal system, numeral 10 is obtained.

The data thus stored is transferred in turn from a first line of #0 bitto a device of next step (e.g. a shift driver operatively connected withthe active matrix electro-optical device), as shown in FIG. 16. When thetransfer is carried out up to an eighth row (line), it is re-startedfrom a first row (line) of #7 bit in turn.

When the transfer of #7 bit is completed, the data is transferred insuch a manner as (#1, #6), (#2, #5), (#3, #4), as shown in FIG. 17. Theorder of the transfer may be reverse thereof, or may be in the order of(#0, #7), (#6, #1), (#2, #5), (#4, #3). In any way, the density of imageoutput is the highest when the combination of the data of #3 and #4 isoutputted, as shown infra, and there will be no particular problem ifthe other data combinations are designed to be of the density lower thanthis combination.

In case of 128 gradations, since the signal is 7-bit from #0 to #6,two-digit signals cannot be coupled with each other. In this case, adigit which does not include an image signal is separately provided as adummy, which may be handled as #7, so as to carry out a process inapparently the same way as for 8-bit. The data #6 can be processedindividually, with the rest properly coupled, in such a way as #6, (#0,#5), (#1, #4), (#2, #3).

When a data is transferred in a single mode in such a way as #0, #1, #2,. . . , in the manner shown in FIG. 2 without making combinations asshown in the abovementioned examples, the technical idea of coupling thedata of higher output density and of lower output density together so asto average the densities, and to maintain a low density, cannot berealized. There will be no problem, however, if the process velocity ofa later step is high enough compared with the transfer velocity of thedata.

The data thus transferred is distributed to each line of Y-line by ashift resister, and is inputted to FIFO, where the data precedentlyinputted is transmitted ahead in turn, and is sent to a LCD driver injust the same way when a gelidium jelly is pushed out one after another,and is thus outputted to each Y-line. This is illustrated in FIG. 18.The velocity is not constant. Referring to FIG. 18, after the data of #0bit is pushed out, the data of #7 bit is pushed out, and after a while,the data of #1 bit is pushed out. This is illustrated in FIG. 19.

Signals of X-line designated by SL 0-7, signals of Y-line designated byDL 0-7, and the data transfer to Y-line, are illustrated in FIG. 19.When the data of #0 is first outputted to Y-line, the data of #7 as wellas of #1 are stored in FIFO. The output of #0 is completed during a timeT, and then the data #7 is outputted, which will be completed during thetime T. The data of #7 is retained on a screen matrix during the time127T. The data of #6, and subsequently the data of #2 are inputted toFIFO via a shift register, while the data #0 and #7 are outputted. Thetime necessary for this process is 12T for each, thus a total 24T. Whenthe data of #1 is outputted, only one-twelfth of the data of #6 isinputted to FIFO, and, even when the data of #7 is outputted, onlyone-sixth of the data input of #6 has been completed. In order to carryout the inputting of these data, the time during which the data of #7 isdisplayed on a screen and a LCD driver is not actuated, is primarilyused. For this reason, the circuit of the former step of FIFO, e.g. ashift register or a memory of digital data for gradation display, can beoperated at a speed lower than that of the LCD driver, and the burden onthe circuit is thus alleviated.

The data of #1 is then outputted, and after the data output iscompleted, the data of #8 is outputted after an interval of a time T.Since a vacancy is generated in FIFO by the data of #1 being outputted,the following data of #5 as well as of #3 are inputted thereto. The timenecessary for the input is 24T, the same as required for the input ofthe data of #6 as well as of #2.

The data of #3 as well as of #4 are inputted to FIFO, and is outputtedfrom an LCD driver in this manner, and one cycle is completed thereby,forming one screen of 256-gradation display. As mentioned supra, thetime required for data input to FIFO was 12T per 1-bit, which will bedetermined in consideration of the time for outputting the data of #3 aswell as of #4. Namely, after the data of #3 stored in FIFO is outputtedduring the time T, as shown in the figure, it is retained during thetime 7T, and subsequently the data of #4 is retained during the time 15Tafter the data of #4 is outputted during the time T. These take placeduring the time 24T, which is shorter than the time for retaining dataof any other combinations. Since the data of #7 as well as of #1 are tobe inputted to FIFO during this time, the maximum velocity for the datatransfer to FIFO is defined as 12 T per 1-bit. The data transfer can becarried out within the time shorter than this.

The explanation supra was related to the FIFO of 24×8 bits, and the sizeof the FIFO is determined in consideration of the size of a matrix of adisplay device: if the size of the matrix is N×M, the size of the FIFOwill be of 3×N×M.

As should be clear from the explanation supra, since fine timeallocation is required in order to carry out high gradation display, avery high-speed switching is essential for the circuit of such as activedevice (TFT), shift register, LCD driver, and of FIFO. In order toachieve 256 gradations, for example, 30 or more of moving picturesshould be fed per second, thus 256T₁ <300 msec, so that T₁ <100 microsecis to be achieved. If X-line which is connected with a gate electrodeconsists of 480 lines, for example, 480 signals must be outputted toeach Y-line in 100 microsec and each X-line has to follow the velocityto drive TFT: consequently, it is required that a pulse of no longerthan 200 nsec. is applied, and that TFT can respond to such pulse.Although only the TFT of NMOS was used in the example shown in FIG. 5,the circuit having a CMOS circuit may be connected to a picture elementfor the purpose of increasing an operational velocity. Namely, CMOSinverter circuit, CMOS modified inverter circuit, CMOS modified buffercircuit, or CMOS modified transfer gate circuit and the like may beused.

The present invention is thus directed to a method of driving anelectro-optical device including the steps of: (a) converting an analogimage signal into digital binary signals of k digits; (b) outputtingdata D_(k-2j+1) in accordance with the digital binary signal S_(k-2j+1)on an active matrix electro-optical device for a period of 2K^(-2j+1) T₁with the digital binary signal S_(2j-1) stored in a first in first outmemory device during duration of the data D_(k-2j+1) on the activematrix electro-optical device where T₁ is a constant period and k and jare integers and j<k/2; (c) transferring the digital binary signalS_(k-2j+2) to the first in first out memory device during the outputtingstep; (d) outputting data D_(2j-1) in accordance with the digital binarysignal of S_(2j-1) on the active matrix electro-optical device for aperiod of 2^(2j-1) T₁ after the data D_(k-2j+1) outputting step; and (e)outputting data D_(k-2j+2) in accordance with the digital binary signalS_(k-2j+2) on said active matrix electro-optical device for a period of2^(k-2j+2) T₁ after the data D_(2j-1) outputting step.

Moreover, the invention is further directed to a method of driving anelectro-optical device including the steps of: (a) converting an analogimage signal into digital binary signals of k digits; (b) outputtingdata D_(k-2j) in accordance with the digital binary signal S_(k-2j) onan active matrix electro-optical device for a period of 2^(k-2j) T₁ withthe digital binary signal S_(2j) stored in a first in first out memorydevice during duration of the data D_(k-2j) on the active matrixelectro-optical device where T₁ is a constant period and k and j areintegers and j<k/2; (c) transferring the digital binary signalS_(k-2j+1) to the first in first out memory device during the outputtingstep; (d) outputting data D_(2j) in accordance with the digital binarysignal S_(2j) on the active matrix electro-optical device for a periodof 2^(2j) T₁ after the data D_(k-2j) outputting step; and (e) outputtingdata D_(k-2j+1) in accordance with the digital binary signal S_(k-) 2j+1on the active matrix electro-optical device for a period of 2^(k-2j+1)T₁ after the data D_(2j) outputting step.

Although there was no description concerning the alternating techniquefor preventing the deterioration of a liquid crystal due to electrolysisetc. under application of dc current to the liquid crystal for a longtime, by reversing the direction of the voltage applied to the liquidcrystal in a cycle for every screen, or for every few screens, sincethis technique does not contradict the present invention, it should beclear that the alternating technique may be carried out in accordancewith the present invention.

Although the non-voltage state and the voltage state of a signal wereclearly discriminated in the explanation supra, for the purpose ofsimplification, the only question is whether the level of the signal isnot more or not less than the thresholds of liquid crystal and of TFT,and the level is not necessarily zero. It should be also clear that thewidth, height, or polarity of a pulse should be determined according tothe operational condition of a device.

It is also possible to change a practical voltage applied to a pictureelement material by applying a proper bias voltage to the counterelectrode of the picture element. For example, by applying a propervoltage to the counter electrode of the picture element, the directionof the voltage applied to the picture element material can be ofpositive or negative as required. This operation is essential when aferroelectric liquid crystal is used.

Although a screen was scanned line by line according to the explanationsupra, the skip scanning method, by which scanning is carried out forevery other line or for every few lines, can be adopted.

Examples of preferred embodiments for manufacturing TFT necessary forimplementing the present invention, as well as for manufacturing a NTSCtype television, are described infra.

Preferred Embodiment 1

In this embodiment, a wall mounted television set was manufactured byusing the liquid crystal device utilizing the circuit structure as shownin FIG. 5, which will be described infra. Polycrystalline silicon thatreceived laser annealing was used for TFT at the time of manufacturing.

The actual arrangement or structure of electrodes etc. corresponding tothis circuit structure is shown in FIG. 6, for one picture element. Themanufacturing method of the liquid crystal panel used in the firstpreferred embodiment will be first explained with reference to FIGS. 7and 8. FIGS. 7 and 8 are cross sectional views and plan views of theliquid crystal panel, respectively. Referring to FIG. 7(A), a siliconoxide film was manufactured at a thickness of 1000-3000 angstroms as ablocking layer 51 by magnetron RF(high frequency) sputtering, on a glasssubstrate 50, which is not expensive such as quartz, and which can bearthe thermal treatment of no more than 700° C., for example,approximately 600° C., under the process conditions as follows: in a100% oxygen atmosphere; the temperature of film formation was 15° C.;output was 400-800 W; and pressure was 0.5 Pa. The rate of filmformation was 30-100 angstroms/minute when quartz or single crystallinesilicon was used as a target.

A silicon film 52 was manufactured thereon by plasma CVD. Thetemperature for film formation was 250°-350° C., or 320° C. in thispreferred embodiment, and mono-silane (SiH₄) was used. Besidesmono-silane (SiH₄), disilane (Si₂ H₆) or trisilane (Si₃ H₈) may be used.These were introduced into a PCVD device at a pressure of 3 Pa, and thefilm was formed by applying high frequency power of 13.56 MHz. At thetime, high frequency power should be 0.02-0.10 W/cm², or 0.055 W/cm² inthis preferred embodiment. The flow rate of mono-silane (SiH₄) was 20SCCM, and the rate of film formation was approximately 120angstroms/minute at the time. The silicon film may be an intrinsicsemiconductor or boron may be added to the film at a concentration of1×10¹⁵ -1×10¹⁸ cm⁻³ by means of diborane during the film formation.Sputtering or low pressure CVD may be employed instead of the plasma CVDfor the formation of the silicon layer which will be a channel region ofTFT, which will be described below in a simplified manner.

In case of sputtering, a single crystalline silicon was used as atarget, and the sputtering was carried out in the atmosphere of 20-80%of hydrogen mixed with argon, with the back pressure before sputteringdefined no more than 1×10⁻⁵ Pa: e.g. 20% of argon and 80% of hydrogen;the temperature for film formation was 150° C.; frequency was 13.56 MHz;sputtering output was 400-800 W; and, pressure was 0.5 Pa.

In case of employing low pressure CVD, disilane(Si₂ H₆) or trisilane(Si₃H₈) was supplied to a CVD device, at a temperature of 450°-550° C.,100°-200° C. lower than the temperature of crystallization, e.g. at 530°C. The pressure in a reactor was 30-300 Pa, while the rate of filmformation was 50-250 angstroms/minute.

Oxygen concentration in the film formed in this way is preferably notmore than 5×10²¹ cm⁻³. The oxygen concentration should be no more than7×10¹⁹ cm⁻³, or preferably no more than 1×10¹⁹ cm⁻³,in order to promotecrystallization however if the concentration is too low, leakage currentin an OFF condition is increased due to the illumination of a backlight, whereas, if the concentration is too high, crystallization willnot be facilitated, and the temperature or time for laser annealing mustbe higher or longer thereby. The concentration of hydrogen was 4×10²⁰cm⁻³, which was one atom % for the silicon at a concentration 4×10²²cm.sup.×3.

Oxygen concentration should be not more than 7×10¹⁹ cm⁻³ or preferablynot more than 1×10¹⁹ cm⁻³, so as to promote crystallization for sourceor drain, while oxygen may be ion-implanted only into the region thatforms a channel of TFT constituting a pixel, at a concentration of5×10²⁰ -5×10²¹ cm⁻³.

The silicon film in an amorphous state was formed at a thickness of500-5000 angstroms, or 1000 angstroms in this preferred embodiment, inthe manner described above.

Patterning was carried out for a photoresist 53 using a first mask 1 soas to open only the region for source or drain. A silicon film 54 wasmanufactured thereon as an n-type activation layer, by plasma CVD, atthe temperature of film formation 250° C.-350° C., e.g. 320° C. in thepreferred embodiment 1, and mono-silane(SiH₄) and phosphine (PH₃) ofmono-silane base at a concentration of 3% were used. These wereintroduced into the PCVD device at a pressure of 5 Pa, and the film wasformed by applying high frequency power of 3.56 MHz. The high frequencypower should be 0.05-0.20 W/cm², e.g. 0.120 W/cm² in the preferredembodiment 1.

The specific electric conductivity of the n-type silicon layer thusformed was approximately 2×10⁻¹ [Ω.cm⁻¹ ], while film thickness was 50angstroms. Thus, the structure shown in FIG. 7(A) was obtained. Theresist 53 was then removed using a lift-off method, and source and drainregions 55 and 56 were formed. Thus, the structure shown in FIG. 7(B)was obtained.

The source, drain and channel regions were laser-annealed by XeClexcimer laser, and the activation layer was laser-doped at the same timeas shown in FIG. 7(C). The threshold energy of the laser energy employedat the time was 130 mJ/cm², and 220 mJ/cm² is necessary as the laserenergy in order to melt the film throughout thickness of the film. Ifthe energy of no less than 220 mJ/cm² is irradiated from the start,however, hydrogen included in the film will be abruptly ejected, and thefilm will be damaged thereby. Thus the melting must be carried out onlyafter hydrogen is first ejected at a low energy. In the first preferredembodiment, crystallization was carried out at an energy of 230 mJ/cm²,after hydrogen was first purged out at 150 mJ/cm².

Then, the silicon film 52 was etched off by a second mask 2 to form anisland region 63 for an N-channel thin film transistor.

A silicon oxide film was formed as a gate insulating film thereon at athickness 500-2000 angstroms, e.g. 1000 angstroms, under the samecondition as for the silicon oxide film manufactured as a blockinglayer. A small amount of fluorine may be added thereto at the time offilm formation, so as to stabilize sodium ion.

Further, a silicon film doped with phosphorus at a concentration1-5×10²¹ cm⁻³, or a multi-layered film comprising this silicon film andmolybdenum (Mo), tungsten (W), MoSi₂ or WSi₂ film formed thereupon, wasformed on the above-mentioned silicon oxide film, which was thensubjected to a patterning process using a third photomask 3. A gateelectrode 66 for NTFT was then obtained, as shown in FIG. 7(D): as agate electrode a phosphorus-doped silicon layer was formed at athickness of 0.2 micrometer and a molybdenum layer was formed thereuponat a thickness of 0.3 micrometer, for example. The channel length wase.g. 7 μm.

At the same time, a gate wiring 65 and a wiring 68 in parallel therewithwere obtained by the patterning as shown in FIG. 8(A).

As a gate electrode material, other material than described above, e.g.aluminum (Al), can be used.

In case of using aluminum (Al) as a gate electrode material, since aself-aligning process is available by anodic-oxidizing the surface ofaluminum that is first patterned by a third photomask 3, the contactholes of source and drain can be formed closer to the gate, and TFTcharacteristic can be improved due to the increase in mobility as wellas the reduction in threshold voltage.

In this way, C/TFT can be manufactured without elevating the temperaturenot less than 400° C., in every process. Therefore, there is no need touse an expensive material such as quartz as a substrate, and it can besaid that this is a most suitable process for manufacturing thewide-screen liquid crystal display device in accordance with the presentinvention.

An inter-layer insulating film 69 made of silicon oxide was formed bysputtering, in the manner described supra. The silicon oxide film can beformed by LPCVD, photo-CVD, or by atmospheric pressure CVD. The film wasformed at a thickness of 0.2-0.6 micrometer, for example, and an opening79 for electrode was formed using a fourth photomask 4. Aluminum wasthen sputtered over all of these at a thickness of 0.3 micrometer, and alead 74 as well as a contact 73 were formed using a fifth photomask 5 asshown in FIG. 7(E) and FIG. 8(B) (plan view), and thereafter an organicresin 77 for flattening or a transparent polyimide resin, for example,was applied to the surface thereof, and an opening of an electrode wasformed again by a sixth photomask 6. An ITO (indium tin oxide) wassputtered over all of these, at a thickness of 0.1 micrometer, and apicture element electrode (pixel electrode) 71 was formed using aseventh photomask 7. The ITO was formed at a temperature ranging fromroom temperature to 150° C., and was then subjected to annealing processin oxygen or atmosphere at a temperature of 200°-400° C. Thus, thestructure shown in FIGS. 7(F) and FIG. 8(C) (plan view) was obtained. InFIGS. 7(F) and 8(C), the thin film transistor is connected with thepixel electrode 71.

The cross section A--A of FIG. 8(C) is shown in FIG. 8(D). In practice,a counter electrode is provided in such a way that a liquid crystalmaterial is sandwiched between the counter electrode and the structureshown in FIG. 8(D), while a capacity is generated between the counterelectrode and a picture element electrode 71, as shown in the figure. Acapacity is also generated between the wiring 68 and the electrode 71 atthe same time. By maintaining the wiring 68 in the same electricpotential as the counter electrode, a circuit in which a capacity isinserted in parallel with a liquid crystal picture element, is to beformed, as shown in FIG. 5. By arranging in accordance with thepreferred embodiment, the effect of reducing the damping or delay of thesignal transmitted in a gate wiring can be obtained, since the wiring 68is placed in parallel with the gate wiring 65, and the level of theparasitic capacity between the two wirings is small.

When the wiring 68 thus formed is to be used in a grounded form, it canbe used as a grounding conductor of a protection network provided on thetailing end of each matrix. The protection network is a circuit as shownin FIG. 11 provided between a peripheral driving circuit and a pictureelement. Examples of the protection circuits are shown in FIGS. 12 and13. Each one will be turned ON when an excessive voltage is applied tothe picture element wiring, and has the function of removing voltagethereby. The protection network is formed out of doped semiconductor,un-doped semiconductor material such as silicon, transparent conductivematerial such as ITO, or of general wiring material. The protectionnetwork thus can be formed at the same time when the circuit of thepicture element is formed.

This should be clear from the fact that the protection networks shown inFIG. 12 are formed out of NTFT or PTFT, or of C/TFT comprising these.Although the protection networks shown in FIG. 13 do not utilize TFT, adiode has a structure of, for example, PIN junction, and, in particular,the diode which is specially known for the Zener effect has a structuresuch as NIN, PIP, PNP, NPN, PINIP or NIPIN, and it goes without sayingthat this can be manufactured by applying the manufacturing methodpresented in the preferred embodiment.

Regarding the electric characteristics of TFT thus obtained, mobilitywas 80 (cm² /Vs), and Vth was 5.0 (V). In this manner, one substrate forthe electro-optical device was manufactured in accordance with thepresent invention.

The arrangement of the electrode, etc., of this liquid crystal displaydevice is shown in FIG. 6. The liquid crystal display device havingpicture elements as many as 640×480, 1280×960, or 1920×400 in thispreferred embodiment, can be obtained by repeating such a structurehorizontally and vertically. In this way, a first substrate wasobtained.

The manufacturing method of the other substrate (a second substrate) isshown in FIG. 10. A polyimide resin for which a black pigment is mixedwith polyimide was formed on a glass substrate at a thickness of 1micrometer by a spin-coating method, and a black stripe 81 wasmanufactured by using an eighth photomask 8, whereafter, the polyimideresin mixed with a red pigment was formed at a thickness of 1 micrometerby the spin-coating method, and a red filter 83 was manufactured using aninth photomask 9. A green filter 85 and a blue filter 86 were formed inthe manner, using masks ○10 and ○11 . Each filter was baked in nitrogenat a temperature of 350° C., for sixty minutes, at the time ofmanufacturing thereof. A leveling layer 89 was then manufactured usingtransparent polyimide, again by spin-coating.

An ITO(indium tin oxide) was then sputtered over all of these at athickness of 0.1 micrometer, and a common electrode 90 was formed usinga twelfth photomask ○12 . The ITO was formed at a temperature rangingfrom room temperature to 150° C., and was subjected to the annealingprocess in oxygen or atmosphere at a temperature of 200°-300° C., and asecond substrate was thus obtained.

A polyimide precursor was then printed on the above-mentioned substrateusing an offset method, and was baked in a non-oxidating atmosphere,e.g. in nitrogen, for an hour, at a temperature of 350° C. It was thensubjected to a known rubbing method, and the quality of the polyimidesurface was modified thereby, and whereby a means for orienting a liquidcrystal molecule in a specific direction at least in an initial stage,was provided.

A nematic liquid crystal composition was sandwiched by the first and thesecond substrates formed in the way as described supra, and theperiphery thereof was fixed with an epoxy bonding agent. Anelectro-optical modulating layer comprising the liquid crystalcomposition was then formed between the first and the second substrates.A PCB having an electric potential wiring, a common signal and a TABdriver IC was connected to the lead on the substrate, while a polarizingplate was adhered to the outside, and a transmission-type liquid crystalelectro-optical device was obtained thereby. A rear lightning deviceprovided with three pieces of cold cathode tubes, and a tuner forreceiving television radio wave, were connected to the liquid crystalelectro-optical device, and the wall mounted television set wascompleted thereby. Since the device has a flatter shape than theconventional CRT television, it can be installed on the wall and thelike. The operation of the present liquid crystal television with 8gradation levels was verified by applying the signal which issubstantially equal to the one shown in FIG. 2, to the liquid crystalpicture element. At this time, T₁ =4 msec. and pulse widths (or shortestpulse widths) applied to X-lines and Y-lines are 5 μsec. and 8 μsec.,respectively.

Preferred Embodiment 2

In this embodiment, a wall mounted television set manufactured by usinga liquid crystal display device having a circuit structure as shown inFIG. 5, will be explained. Polycrystalline silicon subjected to laserannealing was used for TFT.

The manufacturing of a TFT part will be described infra according toFIG. 9. Referring to FIG. 9(A), a silicon oxide film was manufactured asa blocking layer 101 on an inexpensive glass substrate 100 which bearsthe heat treatment of not more than 700° C., e.g. approximately 600° C.,at a thickness of 1000-3000 angstroms by magnetron RF (high frequency )sputtering. The conditions for the process were: in 100% oxygenatmosphere; the temperature for film formation was 15° C.; output was400-800 W; and, pressure was 0.5 Pa. The rate of film formation was30-100 angstroms/min, when quartz or single crystalline silicon was usedas a target.

A silicon film 102 was manufactured thereon by plasma CVD. Thetemperature for film formation was 250° C.-350° C., e.g. 320° C. In thisembodiment, mono-silane (SiH₄). was used, however, disilane (Si₂ H₆) ortrisilane (Si₃ H₈) can be used instead. These were introduced into aPCVD device at a pressure 3 Pa, and the film formation was carried outby applying high frequency power of 13.56 MHz thereto. The highfrequency power should be 0.02-0.10 W/cm², or 0.055 W/cm² in thisembodiment. The flow rate of mono-silane (SiH₄) was 20 SCCM, and therate of film formation was approximately 120 angstroms/min. The siliconfilm may be an intrinsic semiconductor or boron may be added to the filmby means of diborane during the film formation at a concentration of1×10¹⁵ -1×10¹⁸ cm⁻³ 3. When a silicon layer that will be a channelregion of TFT is to be formed, sputtering or low pressure CVD can beemployed instead of plasma CVD, which will be briefly described infra.

In case of sputtering, the back pressure before sputtering should be notmore than 1×10⁻⁵ Pa, and the sputtering was carried out in theatmosphere for which 20-80% of hydrogen was mixed with argon; e.g. 20%of argon and 80% of hydrogen. The target was single crystal silicon. Thetemperature for film formation was 150° C.; frequency was 13.56 MHz;sputtering output was 400-800 W; and, pressure was 0.5 Pa.

In case of carrying out low pressure CVD, film formation was carried outby supplying disilane (Si₂ H₆) or trisilane (Si₃ H₈) to a CVD device ata temperature of 4.50°-550° C., 100°-200° C. lower than the temperaturefor crystallization, e.g. at 530° C. The pressure in a reactor was30-300 Pa. The rate of film formation was 50-250 angstroms/min.

Oxygen in the film thus formed should be not more than 5×10²¹ cm⁻³.Oxygen concentration should be not more than 7×10¹⁹ cm⁻³, or preferablynot more than 1×10¹⁹ cm⁻³, so as to promote crystallization, however, ifit is too low, the leakage current in OFF state will be increased due tothe illumination of a back light, thus the abovementioned level issupposed to be optimum. If oxygen concentration is too high,crystallization will not be facilitated, and the temperature for laserannealing must be higher or the time for laser annealing longer.Hydrogen concentration was 4×10²⁰ cm⁻³, or one atom % compared with thesilicon at a concentration of 4×10²² cm⁻³.

Oxygen concentration should be not more than 7×10¹⁹ cm⁻³, preferably notmore than 1×10¹⁹ cm⁻³, in order to promote crystallization for sourceand drain, and oxygen can be ion-implanted only into channel formingregions of TFTs constituting pixels, at a concentration of 5×10²⁰-5×10²¹ cm⁻³. The silicon film in amorphous state was thus formed by500-5000 angstroms, or by 1000 angstroms in this embodiment.

A photoresist pattern 103 having openings therein only over regions tobe source and drain regions of NTFT was then formed by using a mask 1.Phosphorus ion was ion-implanted at concentrations 2×10¹⁴ -5×10¹⁶ cm⁻²,preferably at 2×10¹⁶ cm⁻² by using the resist 103 as a mask, and n-typeimpurity regions 104 were formed thereby, and the resist 103 was removedthereafter.

A silicon oxide film 107 of 50-300 nm thick, e.g. 100 nm thick was thenformed on the silicon film 102, by the abovementioned RF sputtering asshown in FIG. 9(B). Source, drain and channel regions were crystallizedand activated through laser annealing using a XeCl excimer laser. Thethreshold level of the laser energy was 130 mJ/cm², and 220 mJ/cm² isnecessary so as to melt the entire film. If the energy of no less than220 mJ/cm² is irradiated from the start, the film will be damaged, sincethe hydrogen existing in the film is abruptly ejected. For this reason,the film must be melted only after the hydrogen is purged out first at alow energy. In this embodiment, after hydrogen was purged out at anenergy of 150 mJ/cm², crystallization was carried out at 230 mJ/cm².After the laser annealing was completed, the silicon oxide film 107 wasremoved.

Otherwise, the crystallization can be carried out by thermal annealing.The thermal annealing process may be a heating process at a temperatureof 450° C. to 700° C. , preferably 550° C. to 600° C., for 12 to 70hours, e.g. 24 hours, in a non-oxidating atmosphere, e.g. hydrogen ornitrogen atmosphere.

Island-like NTFT region 111 was then formed by a photomask 2. A siliconoxide film 108 was formed thereupon as a gate insulating film at athickness of 500-2000 angstroms, e.g. 1000 angstroms. The manufacturingconditions were the same as for those of the silicon oxide film as ablocking layer. A little amount of fluorine may be added to the filmduring the manufacturing thereof, so as to stabilize sodium ion.

A silicon film containing therein phosphorus at a concentration of1-5×10²¹ cm⁻³ or a multi-layered film comprising this silicon film and amolybdenum (Mo), tungsten (W), MoSi₂ or WSi₂ film formed thereon, wasformed thereupon. This was patterned by a third photomask 3, to form agate electrode 109 for NTFT as shown in FIG. 9(D). For example, thechannel length was 7 micrometer and as a gate electrode phosphorus-dopedsilicon layer was formed at a thickness of 0.2 micrometer and molybdenumlayer was formed thereon at a thickness of 0.3 micrometer. A gate wiringand a wiring in parallel therewith were formed in the same way as in thecase of the Preferred Embodiment 1.

As a material for these wirings, other material than described above,e.g. aluminum (Al) can be used.

In case of using aluminum (Al) as a gate electrode material, since aself-aligning process is available by anodic-oxidating the surface ofthe aluminum which is primarily patterned by a third photomask 3, thecontact holes of source and drain can be formed closer to the gate, andTFT characteristic is further improved due to the increase in mobilityand the reduction in threshold voltage.

Referring to FIG. 9(E), a silicon oxide film was formed as aninter-layer insulator 113 by sputtering in the way described supra. Thesilicon oxide film can be formed by LPCVD, photo-CVD, or by atmosphericpressure CVD, at a thickness of 0.2-0.6 micrometer, for example, and anopening 117 for electrode was then formed by using a fourth photomask 4.Aluminum was further sputtered over the entire surface of these at athickness of 0.3 micrometer, and, after a lead 116 and a contact 114were manufactured by using a fifth photomask 5, an organic resin 119 forflattening, e.g. a transparent polyimide resin was applied to thesurface thereof, and an opening for an electrode was formed by using asixth photomask 6. An ITO (indium tin oxide) was sputtered on the entiresurface of these at a thickness of 0.1 micrometer, and a picture elementelectrode 118 was formed by using a seventh photomask 7. The ITO wasformed at a temperature ranging from room temperature to 150° C., andwas then subjected to annealing process in atmosphere or in oxygen at atemperature of 200°-400° C.

The electric characteristic of the TFT thus obtained was: mobility of 90(cm² /Vs) and Vth of 4.8 (V).

In this way, a first substrate for the liquid crystal electro-opticaldevice was obtained. The manufacture of the other substrate (a secondsubstrate), which is the same as described in the preferred embodiment1, is omitted here. A nematic liquid crystal composition was thensandwiched by the abovementioned first and second substrates, and theperiphery thereof was fixed by an epoxy bonding agent. PCB having anelectric potential wiring, a common signal, and a TAB-shaped driver ICwere connected to the lead on the substrate, and a polarizing plate wasadhered to the outside, and a transmission type liquid crystalelectro-optical device was thus obtained. A wall mounted television setwas completed by connecting this device with a tuner for receivingtelevision electric wave and a rear lighting device comprising threepieces of cold cathode-ray tubes. Since the device becomes flattercompared with a conventional CRT type television, it can be installed onthe wall and the like. The operation of the liquid crystal televisionwith 128 gradation levels was verified by applying the signalsubstantially the same as the one shown in FIG. 2, to a liquid crystalpicture element.

Preferred Embodiment 3

A device used when an actual monochrome television (NTSC) was driven inaccordance with the present invention, is shown in FIGS. 20, 21 and 23,and examples of driving signals are shown in FIGS. 22 and 24.

A screen of the television and a peripheral circuit thereof are shown inFIG. 20, and the size of the matrix of the screen is 720×480. FIFO isthus of 720×480×3=1036800 bits, and a driver and a shift register ofX-line are of 480 dots, while those of Y-line are of 720 dots. A datashift register of Y-line was of 16 bits×45. The timings of these werecontrolled by a sequence controller of gradation driving of LCD.

A polysilicon TFT CMOS (complementary field effect device) transfer gatecircuit was used to form a matrix of the screen. The schematic circuitdiagram related to the four picture elements is shown in FIG. 23. At thetime of manufacturing, a normal low temperature thermal annealingcrystallization method was adopted. The detailed explanation thereof isomitted. In order to effectively operate such a circuit at a high speed,a pulse which is reversed in its polarity (hereinafter referred to asbipolar pulse) will be applied to the X-line connected with the controlelectrode of the circuit, as shown in FIG. 24. The order of alternatingpolarity, the height, or the width of the bipolar pulse are to bedesigned according to the characteristic of a device. An operationalexample of the transfer gate circuit is shown in FIG. 24, which isbasically the same as the case where a normal NMOS type circuit is used,except that a bipolar pulse is used.

A block figure of the signal process part of the television is shown inFIG. 21. After a normal analog image signal was synchronously separated,it was converted into an 8-bit digital image signal by an analog-digitalconverter (A/D 8bit), and after the signal was temporarily stored in adual port memory of 720 dot×480 dot×8 bit, which served as a data memoryfor each gradation display, the signal was sent to a FIFO of next step,which is different from the FIFO in the periphery of a matrix, in theorder as shown in FIG. 17, and is outputted to a data input terminal asshown in FIG. 20 from the FIFO, via a data set shift register. Amonolithic IC was used for the entire peripheral circuit, and a driveroutput terminal was connected to X-line as well as to Y-line by a knownTAB method.

It is also possible to manufacture the peripheral circuit of a matrix,in particular, a driver, FIFO, or a shift register, out of polysiliconat the same time with the matrix. In this case, since the process ofconnecting a lot of X-lines and Y-lines is not necessary, the productionyield can be improved, while the price can be reduced.

The signal to be applied to the circuit is shown in FIG. 22. The pulsewidth of the signal applied to X-line was defined as 135 nsec. Since a16-bit data bus was used for the data transfer to the data shiftregister, a pulse of 21600 clock was used for the transfer of the data(720×480) per 1-bit. The time for data transfer per 1-bit was defined as780 microsec, while no signal was applied, for example, between the dataof #6 and the data of #2, only for 3 microsec. The frequency of the datafor that purpose was 27.7 MHz. In this manner, the monochrome projectedimage of 256 gradations was obtained by the liquid crystal device.

The present invention is characterized by the digital method ofgradation display, compared with a conventional analog method ofgradation display. In case of a liquid crystal electro-optical devicehaving 640×400 dots of picture elements, it was with enormous difficultyto manufacture the device without difference in characteristic of everyTFT that amounts to total 256,000 pieces, and in practice, a 16gradations display is assumed to be an upper limit in consideration ofmass productivity and yield. However, the display of not less than 256gradations has become possible according to the present invention,without applying any analog signal at all, but through completelydigital control. There are no ambiguity in gradation due to differencein characteristics of TFTs, for this method is a completely digitaldisplay, and even if there is any difference in characteristics of TFTsto some extent, a thoroughly homogeneous gradation display is possible.Since there is no more substantial problem with regard to difference incharacteristic of TFT, according to the present invention, compared witha conventional method where there was substantial problem of poor yieldat the time of manufacturing TFTs of little difference in itscharacteristics, the yield of the TFT is improved, while a manufacturingcost is drastically reduced, according to the present invention.

In case of carrying out conventional analog gradation display by aliquid crystal electro-optical device which is composed of 256,000groups of TFTs of 640×400 dots in a 300 mm square, a 16 gradationsdisplay was an upper limit, for there was difference in characteristicsof the TFTs by approximately ±10%. When a digital gradation display iscarried out in accordance with the present invention, a 256 gradationsdisplay is possible, and a various and subtle color display of as manyas 16,777,216 colors is achieved, being little influenced by differencein the characteristics of TFT devices. When a software of such as atelevision image is to be projected, a "rock", for example, of the samecolor should be subtly different in its color due to a lot of very smallrecesses and the like thereupon. When a display as close to the natureas possible is to be carried out, it is difficult with a 16-gradationdisplay, however, the fine variation in color tone has become possiblewith the gradation display in accordance with the present invention.

Although the TFT utilizing silicon was primarily explained in thepreferred embodiment in accordance with the present invention, the TFTutilizing germanium can be used in the same way. A single crystallinegermanium is a most suitable material for implementing the presentinvention that requires high-speed operation, since the characteristicsthereof exceed those of single crystalline silicon. Electron mobility ofsingle crystalline germanium is 3600 cm² /Vs, Hall mobility thereof is1800 cm² /Vs, whereas electron mobility of single crystalline silicon is1350 cm² /Vs, and Hall mobility thereof is 480 cm² /Vs. The transitiontemperature of germanium from an amorphous state to crystal state, islower than that of silicon, which means that germanium is suitable forlow temperature process. The generation ratio of crystal nucleus at thetime of growing germanium crystal is low, which means, in general, alarge crystal can be obtained when it is grown into polycrystallinestate. Germanium has thus a characteristic that can bear comparison withsilicon's.

Although an electro-optical device utilizing liquid crystal, and, inparticular, a display device utilizing liquid crystal are primarilyreferred to in order to explain a technical idea of the presentinvention, the idea of the present invention can be applied to aprojection type television, as well as to other devices such as aphotoswitch or a photoshutter, instead of display device. And it shouldbe also clear that the present invention can be implemented by using anyelectro-optical material which is changed in its optical characteristicwhen electrically affected by electric field, voltage and so on, insteadof by using liquid crystal. It is also clear that the present inventioncan be implemented by using other operational mode of liquid crystalincluding, for example, a guest-host mode, than the mode explainedsupra.

The foregoing description of preferred embodiments has been presentedfor purposes of illustration and description. It is not intended to beexhaustive or to limit the invention to the precise form described, andobviously many modifications and variations are possible in light of theabove teaching. The embodiments were chosen in order to explain mostclearly the principles of the invention and its practical applicationthereby to enable others in the art to utilize most effectively theinvention in various embodiments and with various modifications as aresuited to the particular use contemplated. An example of suchmodifications is as follows.

FIG. 25 is a copy of a photograph showing an electric circuit which wasactually manufactured in accordance with the present invention. Theelectric circuit shown in FIG. 25 is a modification of the electriccircuit shown in FIG. 23 and is different from the electric circuitshown in FIG. 2 in that no capacitor is provided in parallel with apicture element in the electric circuit shown in FIG. 25.

What is claimed is:
 1. A method of driving an electro-optical devicecomprising the steps of:applying pulses to a signal line at intervals,wherein said intervals are T₁ between the i-th pulse and the (i+1)-thpulse, 2^(N) T₁ between the (i+1)-th pulse and the (i+2)-th pulse, 2T₁between the (i+2)-th pulse and the (i+3)-th pulse, and 2^(N-i) T₁between the (i+3)-th pulse and the (i+4)-th pulse where N is a naturalnumber, i is a natural number and T₁ is a constant period.
 2. The methodof claim 1 wherein said pulses are rectangular pulses.
 3. The method ofclaim 1 where N=3.
 4. A method of driving an electro-optical devicecomprising the step of:outputting an j-th image signal on an activematrix electro-optical device (j+1)-th and (j+2)-tj image signals bringstored in a first in first out memory device connected to said activematrix electro-optical device during the duration of said j-th imagesignal on said active matrix electro-optical device where j is anarbitrary natural number and where the duration of the j-th image signalis T₁, the duration of the (j+1)-th image signal is 2^(N) T₁, and theduration of the (j+2)-th image signal is 2T₁, N being a natural numberand T₁ being a constant period; and outputting the (j+1)-th image to theactive matrix electro-optical device, (j+2)-th and (j+3)-th imagesignals being stored in the first in first out memory device during theduration of said (j+1)-th image signal on the active matrixelectro-optical device where the duration of the (j+3)-th image signalis 2^(N-1) T₁.
 5. A method of driving an electro-optical devicecomprising the steps of:converting an analog image signal into digitalbinary signals of k digits; outputting data D_(k-2j+1) in accordancewith the digital binary signal S_(k-2j+1) on an active matrixelectro-optical device for a period of 2^(k-2j+1) T₁ with the digitalbinary signal S_(2j-1) stored in a first in first out memory deviceduring duration of said data D_(k-2j+1) on said active matrixelectro-optical device where T₁ is a constant period and k and j areintegers and j<k/2; transferring the digital binary signal S_(k-2j+2) tosaid first in first out memory device during said outputting step;outputting data D_(2j-1) in accordance with the digital binary signalS_(2j-1) on said active matrix electro-optical device for a period of2^(2j) -1 T₁ after said data D_(k-2j+1) outputting step; and outputtingdata D_(k-2j+2) in accordance with the digital binary signal S_(k-2j+2)on said active matrix electro-optical device for a period of 2^(k-2j+2)T₁ after said data D_(2j-1) out putting step.
 6. The method of claim 5wherein k is even.
 7. The method of claim 5 wherein said electro-opticaldevice comprises said active matrix electro-optical device, a circuitfor driving said active matrix electro-optical device, said first infirst out memory device connected with said circuit, and a shift driverconnected with said first in first out memory device.
 8. The method ofclaim 5 wherein each of said digital binary signals has a voltage levelselected from the group consisting of a high voltage level and a lowvoltage level.
 9. The method of claim 8 wherein said low voltage levelis a zero level.
 10. A method of driving an electro-optical devicecomprising the steps of:converting an analog image signal into digitalbinary signals of k digits; outputting data D_(k-2j) in accordance withthe digital binary signal S_(k-2j) on an active matrix electro-opticaldevice for a period of 2^(k-2j) T₁ with the digital binary signal S_(2j)stored in a first in first out memory device during duration of saiddata D_(k-2j) on said active matrix electro-optical device where T₁ is aconstant period and k and j are integers and j<k/2; transferring thedigital binary signal S_(k-2j+1) to said first in first out memorydevice during said outputting step; outputting data D_(2j) in accordancewith the digital binary signal S_(2j) on said active matrixelectro-optical device for a period of 2^(2j) T₁ after said dataD_(k-2j) outputting step; and outputting data D_(k-2j+1) in accordancewith the digital binary signal S_(k-2j+1) on said active matrixelectro-optical device for a period of 2^(k-2j+1) T₁ after said dataD_(2j) outputting step.
 11. The method of claim 10 wherein k is even.12. The method of claim 10 wherein said electro-optical device comprisessaid active matrix electro-optical device, a circuit for driving saidactive matrix electro-optical device, said first in first out memorydevice connected with said circuit, and a shift driver connected withsaid first in first out memory device.
 13. The method of claim 10wherein each of said digital binary signals has a voltage level selectedfrom the group consisting of a high voltage level and a low voltagelevel.
 14. The method of claim 13 wherein said low voltage level is azero level.
 15. A method of driving an electro-optical device comprisingthe steps of:converting an analog image signal into digital binarysignals of k digits; storing the digital binary signal of each of said kdigits into corresponding one of memory areas; and sending the digitalbinary signals from said memory areas to a shift driver operativelyconnected with an active matrix electro-optical device so that pulsesare applied to a signal line of the active matrix electro-optical deviceat intervals wherein said intervals are T₁ between the i-th pulse andthe (i+1)-th pulse, 2^(N) T₁ between the (i+1)-th pulse and the (i+2)-thpulse, 2T₁ between the (i+2)-th pulse and the (i+3)-th pulse, and2^(N-1) T₁ between the (i+3)-th pulse and the (i+4)-th pulse where N isa natural number, i is a natural number and T₁ is a constant period. 16.The method of claim 15 wherein k is even.
 17. The method of claim 15wherein said electro-optical device comprises said memory areas, saidactive matrix electro-optical device, a circuit for driving said activematrix electro-optical device, a first in first out memory deviceconnected with said circuit, and said shift driver connected with saidfirst in first out memory device.